O + 5 8 6 1114010.(1S) 1 1s22s(2S) (2)0( 0.5) 0. 2 1s22p(2P) (2)1( 2.5) 96914. 3 1s23s(2S) (2)0( 0.5) 638685. 4 1s23p(2P) (2)1( 2.5) 664879. 5 1s23d(2D) (2)2( 4.5) 672931. 6 1s24s(2S) (2)0( 0.5) 851024. 7 1s24p(2P) (2)1( 2.5) 861696. 8 1s24d(2D) (2)2( 4.5) 865067. 9 1s24f(2F) (2)3( 6.5) 865191. -1 6.00 3 3.60+04 7.20+04 1.80+05 3.60+05 7.20+05 1.80+06 3.60+06 7.20+06 2 1 4.21+08 5.05+00 5.17+00 5.50+00 5.94+00 6.54+00 7.64+00 8.72+00 9.98+00 3 1 0.00+00 2.86-01 2.44-01 2.04-01 1.87-01 1.81-01 1.84-01 1.92-01 2.00-01 4 1 2.58+10 1.57-01 1.46-01 1.39-01 1.41-01 1.56-01 2.16-01 3.02-01 4.27-01 5 1 0.00+00 2.51-01 2.64-01 2.78-01 2.90-01 3.15-01 3.77-01 4.38-01 4.95-01 6 1 0.00+00 4.64-02 4.01-02 3.46-02 3.25-02 3.21-02 3.34-02 3.53-02 3.72-02 7 1 1.21+10 5.86-02 5.32-02 4.59-02 4.28-02 4.38-02 5.45-02 7.18-02 9.76-02 8 1 0.00+00 6.57-02 6.37-02 5.91-02 5.69-02 5.77-02 6.50-02 7.38-02 8.23-02 9 1 0.00+00 4.55-02 4.38-02 3.84-02 3.46-02 3.25-02 3.21-02 3.26-02 3.32-02 3 2 1.68+10 7.38-01 5.17-01 3.07-01 2.14-01 1.64-01 1.49-01 1.71-01 2.15-01 4 2 0.00+00 1.24+00 1.04+00 8.86-01 8.05-01 7.56-01 7.45-01 7.66-01 7.94-01 5 2 8.77+10 2.31+00 2.34+00 2.42+00 2.55+00 2.85+00 3.67+00 4.68+00 6.02+00 6 2 6.41+09 1.08-01 8.34-02 5.83-02 4.48-02 3.58-02 3.04-02 3.12-02 3.58-02 7 2 0.00+00 2.67-01 2.44-01 2.05-01 1.79-01 1.62-01 1.52-01 1.52-01 1.56-01 8 2 2.91+10 4.85-01 4.80-01 4.66-01 4.72-01 5.07-01 6.21-01 7.68-01 9.67-01 9 2 0.00+00 2.51-01 2.38-01 1.99-01 1.72-01 1.56-01 1.53-01 1.61-01 1.72-01 4 3 5.13+07 3.06+01 3.24+01 3.61+01 4.05+01 4.63+01 5.58+01 6.39+01 7.24+01 5 3 0.00+00 4.18+00 3.96+00 3.68+00 3.42+00 3.22+00 3.07+00 3.01+00 2.98+00 6 3 0.00+00 1.09+00 9.35-01 8.32-01 8.19-01 8.44-01 9.08-01 9.59-01 1.00+00 7 3 3.05+09 4.36-01 4.09-01 3.99-01 4.48-01 5.76-01 9.07-01 1.29+00 1.78+00 8 3 0.00+00 7.58-01 7.74-01 8.05-01 8.72-01 9.83-01 1.17+00 1.31+00 1.42+00 9 3 0.00+00 1.00+00 1.01+00 9.95-01 9.99-01 1.02+00 1.05+00 1.07+00 1.08+00 5 4 1.20+06 6.01+01 6.20+01 6.79+01 7.66+01 8.84+01 1.06+02 1.20+02 1.33+02 6 4 4.43+09 1.35+00 9.54-01 6.78-01 6.28-01 7.02-01 9.81-01 1.32+00 1.75+00 7 4 0.00+00 2.74+00 2.67+00 2.63+00 2.72+00 2.91+00 3.28+00 3.57+00 3.81+00 8 4 8.95+09 3.93+00 4.02+00 4.31+00 4.99+00 6.27+00 9.09+00 1.21+01 1.58+01 9 4 0.00+00 4.15+00 4.28+00 4.48+00 4.85+00 5.45+00 6.41+00 7.10+00 7.63+00 6 5 0.00+00 2.39+00 1.52+00 8.22-01 5.35-01 3.78-01 2.83-01 2.54-01 2.43-01 7 5 6.01+08 2.14+00 1.89+00 1.46+00 1.18+00 9.99-01 9.20-01 9.66-01 1.08+00 8 5 0.00+00 5.85+00 5.72+00 5.26+00 4.99+00 4.94+00 5.15+00 5.38+00 5.59+00 9 5 1.79+10 1.96+01 2.05+01 2.23+01 2.54+01 3.05+01 4.08+01 5.13+01 6.38+01 7 6 1.17+07 9.54+01 1.01+02 1.15+02 1.36+02 1.64+02 2.05+02 2.37+02 2.68+02 8 6 0.00+00 1.49+01 1.47+01 1.41+01 1.37+01 1.35+01 1.32+01 1.30+01 1.28+01 9 6 0.00+00 3.13+00 2.95+00 2.46+00 2.11+00 1.88+00 1.72+00 1.67+00 1.65+00 8 7 3.75+05 1.69+02 1.91+02 2.47+02 3.12+02 3.85+02 4.79+02 5.43+02 6.01+02 9 7 0.00+00 2.10+01 2.02+01 1.81+01 1.66+01 1.54+01 1.42+01 1.35+01 1.30+01 9 8 1.14+01 3.40+02 4.09+02 5.17+02 6.05+02 6.90+02 7.85+02 8.45+02 8.98+02 -1 -1 -1 C------------------------------------------------------------------------------- C C See: Griffin D C, Badnell N R, and Pindzola M S 2000 J. Phys. B C 33, 1013 for a more complete description. C C From a 41-state RMPS calculation that included the 9 spectroscopic C terms of the configurations 1s22s, 1s22p, 1s23s, 1s23p, 1s23d, 1s24s, C 1s24p, 1s24d, 1s24f; and the 32 pseudo states 1s2nl for n = 5 to 12 C and l = 0 to 3 in the close-coupling expansion. C C The 1s and 2s orbitals were generated from a single-configuration C Hartree-Fock (SCHF) calculation on 1s22s, while the 2p through 4f C orbitals were generated from a SCHF calculation on the terms C 1s2nl with the 1s orbital frozen. The pseudo states were generated C from an non-orthogonal Laguerre basis; these states were then C orthogonalized with respect to the Hartree-Fock orbitals and each C other. C C For the L = 0 to 12 even and odd parity LSPI partial waves, we C performed an R-Matrix calculation with exchange. For the higher C partial waves we performed a no-exchange R-Matrix calculation for C L = 13 to 60 with the long-range perturbations turned on and with C topup. The continuum basis for these calculations was set to 38 C and the radius of the R-matrix box was 13.96 a.u. C C Donald C. Griffin May 18, 2000 C-------------------------------------------------------------------------------